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Self Evaluation - Nptel

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Lesson 26

1. Can Green’s third identity be directly used to find a solution to Laplace’s equation?

2. If  is a solution to Laplace’s equation, why is n,n1 also a solution?

3. What is Green’s function? Write down the solution of Laplace’s equation in terms of Green’s function?

The function G in the above equation is a Green’s function.

equation.

s Laplace' of

solution the

find o directly t used

be o identity t third

s Green'

prevents This

posed.

- ill problem

the make likely to

is both specifying

boundary,

at the known

are function

or the derivative

e either th

practice in

However

result.

this using domain

out the through

determine

to possible

is it boundary

at the

s derivative

normal its as well as know we if that suggests identity

third s Green'

equation.

s Laplace'

of solutions

are ....

1 ˆ as well as ˆ Hence ˆ 0.

then ˆ 0,

i.e.

solution,

a is

ˆ if constant,

are ts coefficien

the and equation linear

a is equation

s Laplace'

Since

2

2       

    nn

 

 

 

 

 

 

 

V y V

y V

V

y V

V

d G n dS

G G n

n dS G G n

d G

R

n dS G G n

R d G

V U

U

R R U

G ψ

y x

x y

y x y

y

y x

y

 

 

 

 

 

2 2

2 2

2 2

) (

) ( Therefore,

) (

) (

: Hence . ) ( 4 )

( 1 solution, l

fundamenta the

from But

) (

4 ) ( 1

: get we , domain in

0

i.e.

in harmonic

is

and

|

| where 4

1 write we if identity

second s Green' In

(2)

4. How can the Green’s function be used to find solutions of Laplace’s equation?

5. What are spherical harmonics and why are they useful in finding solutions to Laplace’s equation?

In certain physical problems, the solution to Laplace’s equation is best expressed in terms of a series solution. For example, for the case of a spherical inclusion moving with a velocity u in an infinite fluid medium which is otherwise motionless, and the fluid is incompressible as well as irrotational, the resultant motion of the fluid can be found by solving Laplace’s equation.

6. What is Lengendre’s equation and when does it arise?

The solution to Laplace’s equation in a spherical domain can also be obtained by seeking a solution in the separated form:

This gives rise to Legendre’s equation and yields a series expansion in terms of spherical harmonics that involves Legendre’s polynomials.

. on prescribed

conditions boundary

Neumann

have must

i.e.

on known

be must case, In this . )

( : using found be

can 0 for

solutions then

, on 0 such that

find can we if Similarly

on prescribed

conditions boundary

Dirichlet

have must that is t requiremen only

The . )

( : above the from

find can we , 0

case in then , on 0 such that

find can we If

2 2

V n V

ndS G

n V G G

V ndS

G

V G

G

y V

V

y

 

 

 

 

 

 

x x

r r

r

A r n

n

n 1

) (

1) ( 1)

( 1)

( )

(

: solution series

a as expressed be

can then

) ( for expression

final The

1 ) ( 2

) 2 ( )

1 ( )

0 ( ) 0 (

x x

x

x A A A

x

x

 

.equation.

s Laplace'

of

solution

a is series in the Each term .

,

components

has while

components with

vector a

is scalar, a is

2 33 2

21 2 13 2 12 2 11

) 2 ( 1

3 1 2 1 1 )

1 ( )

0 (

} A , A ,A ,A {A

} ,A ,A {A A

) ( ) ( ) ( ) ( ) (

) ( ) ( ) (

A A

harmonics

spherical

as known

are 2 , 1 , 0 1), ( equation,

s Laplace'

to solutions

of set

The  n 

r

n

) (

~) ( )

(r HIG

φ

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